Astrophysics Seminar October 2004 R. L. Mutel (& D. Menietti) University of Iowa Fine Structure in Auroral Kilometric Radiation: Evidence for Electromagnetic and Electrostatic Ion Cyclotron Waves
UI Space/Astro Seminar October 2004 Earth as a radio source
UI Space/Astro Seminar October 2004 AKR is generated km above the visible aurora AKR is generated at f = ω ce by electron cyclotron maser
UI Space/Astro Seminar October 2004 Dynamic Spectra of Common AKR Bursts Geotail Cluster
UI Space/Astro Seminar October 2004 May 15 AKR Event: Variation with Magnetic Latitude m = -53° m = -38° m = -32°
UI Space/Astro Seminar October 2004 Example of WBD Dynamic Spectra ( KHz, 30 sec), S/C separation ~300 km Auroral Kilometric Radiation (AKR) Bursts Spacecraft 1 3 4
UI Space/Astro Seminar October 2004 FAST Observations of AKR Source Region (Ergun et al. Ap. J. 538, 456) Note e - depletion in auroral cavity
UI Space/Astro Seminar October 2004 FAST Observations of AKR Source Region (Ergun et al. Ap. J. 538, 456) Shell instability
UI Space/Astro Seminar October 2004 University of Iowa Wideband Data Plasma Wave Instrument (WBD) Identical WBD instruments are mounted on all four spacecraft. Single dipole antenna used. Real-time downlink of 220 kb/s to the NASA Deep Space Network (DSN). (One DSN antenna per S/C!) DSN provides real-time time stamps (accuracy 10 s). AKR studies use 125, 250, and 500 KHz bands, 10 KHZ bandwidth, 37 s sampling time. High frequency/time resolution capability of WBD is the primary characteristic that makes WBD unique from the other Cluster wave experiments, which operate at much lower data rates.
UI Space/Astro Seminar October 2004 VLBI Source Location Algorithm: Differential delay measurement
UI Space/Astro Seminar October 2004 Sample Dynamic Spectrum, Waveform and Cross-correlation Waveforms from each Cluster WBD receiver for AKR burst shown at left Peak is fit with Gaussian, delay uncertainty ~ 0.3 ms
UI Space/Astro Seminar October 2004 A uniform 3-d grid of points is constructed centered on the Earth with spacing 0.1 Re and dimension 8 Re on each side (512,000 pts). The propagation time to each satellite is computed from each grid point. Differential delays are then computed for each baseline and compared with the observed delays, as measured by cross- correlating the waveforms from each pair of spacecraft AKR Burst Position search algorithm
UI Space/Astro Seminar October 2004 VLBI position uncertainty calculation Delay uncertainties in plane and parallel to line of sight: Typical uncertainty in plane: Typical uncertainty in plane:
UI Space/Astro Seminar October 2004 Uncertainty mapped to Earth (CGM coordinates) Uncertainty ~ 500 km km Uncertainty ~ 200 km -400 km
UI Space/Astro Seminar October 2004 Refractive effects effect on AKR burst location determination unimportant for S/C magnetic latitudes > 40° (plasmasphere model Gallagher et al.2000)
UI Space/Astro Seminar October 2004 Refractive Ray tracing corrections
UI Space/Astro Seminar October 2004 AKR Bursts: Locus of Allowed Locations Locus of allowed locations for AKR burst on 10 July 2002 at 08:47:02 and illustrated at right. The top panels show the unconstrained solution of all allowed points (left is oblique view; right view is from spacecraft). The lower panel shows the constrained solution assuming the AKR emission arises from a radius distance from Earth consistent with the observed frequency being identified with the electron gyrofrequency. A model auroral oval is shown for reference.
UI Space/Astro Seminar October 2004 AKR Burst Locations: The movie
UI Space/Astro Seminar October 2004 Summary of 4 Spacecraft VLBI Epochs (Fully Analyzed)
UI Space/Astro Seminar October 2004 November 9 Locations: Varying Perspectives (Animation)
UI Space/Astro Seminar October 2004 Nov 9 :The Movie Mapped onto CGM coordinates
UI Space/Astro Seminar October 2004 Observed distribution of AKR bursts
UI Space/Astro Seminar October 2004 AKR Burst locations vs.
UI Space/Astro Seminar October 2004 Example of position uncertainty including depth-of-field (9 Oct 02) Blue: f gyro – 10% Red: f gyro + 10%
UI Space/Astro Seminar October 2004 Example of AKR Burst location with Uncertainties projected into 100km Altitude, CGM coordinates (29 Dec 02)
UI Space/Astro Seminar October 2004 Polar Average Images of Northern Auroral by month (Liou et al. 1997) Evening Peak ~22h MLT April -May Day peak at ~15h MLT June -July
UI Space/Astro Seminar October 2004 Summary of 4 Spacecraft VLBI Epochs (Fully Analyzed)
UI Space/Astro Seminar October 2004 Histogram of AKR Burst Locations CGM coordinates, 5 epochs Southern hemisphere only
UI Space/Astro Seminar October 2004 November 9 Locations: Varying Perspectives (Animation)
UI Space/Astro Seminar October 2004 Nov 9 :The Movie Mapped onto CGM coordinates
UI Space/Astro Seminar October 2004 Observed distribution of AKR bursts
UI Space/Astro Seminar October 2004 AKR Burst locations vs.
UI Space/Astro Seminar October 2004 Example of position uncertainty including depth-of-field (9 Oct 02) Blue: f gyro – 10% Red: f gyro + 10%
UI Space/Astro Seminar October 2004 Example of AKR Burst location with Uncertainties projected into 100km Altitude, CGM coordinates (29 Dec 02)
UI Space/Astro Seminar October 2004 Polar Average Images of Northern Auroral by month (Liou et al. 1997) Evening Peak ~22h MLT April -May Day peak at ~15h MLT June -July
UI Space/Astro Seminar October 2004
AKR burst mean location drift: example1 19 Aug 2002, Southern hemisphere
UI Space/Astro Seminar October 2004 AKR burst mean location drift: example2 22 Jan 2003, N hemisphere
UI Space/Astro Seminar October 2004 First simultaneous AKR/VLBI location map with UV image (IMAGE). June 8, 2004 AKR burst is associated with discrete auroral arc
UI Space/Astro Seminar October 2004 ‘Rain’ AKR bursts: Narrow, rapidly drifting structures “normal” AKR burst “Rain” AKR bursts
UI Space/Astro Seminar October 2004 AKR Dynamic Spectrum 125 KHz 17 July :42:30 – 11:43:00 Slope -8.7 KHz/sec
UI Space/Astro Seminar October 2004 AKR Dynamic Spectrum 125 KHz 17 July :42:30 – 11:43:00 Slope = -3.1 KHz/sec
UI Space/Astro Seminar October 2004 Rain AKR bursts at 125 KHz 31Aug :14:30-16:15:00 UT Modulated periodic structures Slope -6.3 KHz/sec
UI Space/Astro Seminar October 2004 Rain AKR bursts at 500 KHz 31Aug :26:00- 19:26:30 UT Slope KHz/sec
UI Space/Astro Seminar October 2004 Derived Speed compared with Alfven, and Electron, Ion Acoustic speeds versus Radial distance (assumes keV particles) Ion acoustic speed Electron acoustic speed Alfven speed 500 KHz250 KHz125 KHz
UI Space/Astro Seminar October 2004 Derived Exciter speed along B field 125 KHz 500 KHz
UI Space/Astro Seminar October 2004 Exitor speed derived from frequency drift 2. Use (negative) frequency drift to derive (upward) wave speed 1. Assume EM at electron gyro-frequency, dipolar magnetic field 3. Recast in terms of f obs 4. Amplitude modulation conversion to spatial wavelength
UI Space/Astro Seminar October 2004 Striated AKR from KHz (Menietti et al. 2000) Slope ~ 1 KHz Slope ~ 0.5 KHz
UI Space/Astro Seminar October 2004
Modulation of Striated AKR: Is it due to Faraday rotation? Requires: Linearly polarized emission (but AKR is circularly polarized) Δ ≈ KHz (λ=2.4 km) => RM = rad-m -2 This may be plausible: B ~ 0.1 gauss, n e ~ 10 cm -3, L ~ 100 km
UI Space/Astro Seminar October 2004
Sampled at 1024 channels
UI Space/Astro Seminar October 2004 Sampled at 2048 channels
UI Space/Astro Seminar October 2004 Wavelet dynamic spectrum of Striated bursts, 2 spacecraft correlation
UI Space/Astro Seminar October 2004 Electromagnetic Ion-Cyclotron Wave Group Speed vs. Frequency where Note: Plot assumes Dipolar B field N e (r) ~ r -3.2 (Persoon model)
UI Space/Astro Seminar October 2004 Banded Modulation of AKR: Evidence for Electrostatic Ion Cyclotron (EIC) Waves?
UI Space/Astro Seminar October 2004 Close-up of AKR banded modulation Separation = 120 ± 5 Hz
UI Space/Astro Seminar October 2004
What excites rain AKR? Model assumptions Observed emission is same as ‘normal’ AKR: electron cyclotron maser near electron cyclotron frequency Earth’s magnetic field is strictly dipolar (OK for r < 2.5 Re) A disturbance traveling parallel to B stimulates EM emission Observed slope indicates phase speed of wave along B field Observed banded modulation may indicates characteristic wavelength of exciter (after conversion to spatial separation)